Abstract
Superconductivity remains one of the most interesting problems in Solid State Physics. During the last years in particular high-transition temperature superconductivity in the cuprates with non-s-wave pairing symmetry and unconventional superconductivity in the isostructural strontiumruthenate (Sr2RuO4) also with a non-s-wave symmetry of the superconducting order parameter and triplet Cooper-pairing have been studied. Cuprates and ruthenates have an oxide layered structure with CuO2-and RuO2-planes, respectively. These seem to play an important role regarding superconductivity and magnetic activity. For an illustration we show in Fig. 9.1 the crystal structures (in Sr2RuO4 the basic element is a RuO2-plane and the superconducting transition temperature for triplet pairing is T c =1.5K). Undoped La2CuO4 is an antiferromagnetic insulator. Superconductivity occurs only upon doping (Ba instead of La) and reaches a maximum for hole doping x = 0.15 with a transition temperature T c ≈ 40K [1]. The different behavior of Sr2RuO4 and La2−x Ba x CuO4 is definitely related to the electronic structure of RuO2 and CuO2-planes.
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Manske, D., Eremin, I., Bennemann, K.H. (2004). Electronic Theory for Superconductivity in High-T c Cuprates and Sr2RuO4 . In: Bennemann, K.H., Ketterson, J.B. (eds) The Physics of Superconductors. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-18914-2_9
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